Mems sensor with decoupled drive system

ABSTRACT

In a first aspect, the angular rate sensor comprises a substrate and a rotating structure anchored to the substrate. The angular rate sensor also includes a drive mass anchored to the substrate and an element coupling the drive mass and the rotating structure. The angular rate sensor further includes an actuator for driving the drive mass into oscillation along a first axis in plane to the substrate and for driving the rotating structure into rotational oscillation around a second axis normal to the substrate; a first transducer to sense the motion of the rotating structure in response to a Coriolis force in a sense mode; and a second transducer to sense the motion of the sensor during a drive mode. In a second aspect the angular rate sensor comprises a substrate and two shear masses which are parallel to the substrate and anchored to the substrate via flexible elements.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims benefit under 35 USC 119(e) of U.S. Provisional Patent Application No. 62/001,474, filed on May 21, 2014, entitled “MEMS SENSOR WITH DECOUPLED DRIVE SYSTEM”, is a continuation-in-part of U.S. patent application Ser. No. 14/041,810, filed Sep. 30, 2013, (IVS-212/5290P) entitled “MICROMACHINED GYROSCOPE INCLUDING A GUIDED MASS SYSTEM,” and is a continuation-in-part of U.S. patent application Ser. No. 14/472,143, filed Aug. 28, 2014, (IVS-147C/5007C) entitled “MICROMACHINED GYROSCOPE INCLUDING A GUIDED MASS SYSTEM,” which is a continuation application and claims priority to U.S. application Ser. No. 13/235,296, filed Sep. 16, 2011, (IVS-147/5007P) entitled “MICROMACHINED GYROSCOPE INCLUDING A GUIDED MASS SYSTEM,” all of which are incorporated herein by reference in their entireties.

FIELD OF THE INVENTION

The present invention relates generally to angular velocity sensors and more particularly relates to angular velocity sensors that include guided mass systems.

BACKGROUND

Sensing of angular velocity is frequently performed using vibratory rate gyroscopes. Vibratory rate gyroscopes broadly function by driving the sensor into a first motion and measuring a second motion of the sensor that is responsive to both the first motion and the angular velocity to be sensed.

Accordingly, what is desired is to provide a system and method that overcomes the above issues. The present invention addresses such a need.

SUMMARY

An angular rate sensor is disclosed. In a first aspect, the angular rate sensor comprises a substrate and a rotating structure anchored to the substrate. The angular rate sensor also includes a drive mass anchored to the substrate and an element coupling the drive mass and the rotating structure. The angular rate sensor further includes an actuator for driving the drive mass into oscillation along a first axis in plane to the substrate and for driving the rotating structure into rotational oscillation around a second axis normal to the substrate; a first transducer to sense the motion of the rotating structure in response to a Coriolis force in a sense mode; and a second transducer to sense the motion of the sensor during a drive mode.

In a second aspect, the angular rate sensor comprises a substrate and a first shear mass and a second shear mass which are parallel to the substrate and anchored to the substrate via at least a first plurality of flexible elements. The angular rate sensor further includes a drive mass which is parallel to the substrate and anchored to the substrate via at least a second plurality of flexible elements.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A illustrates a first embodiment of a single axis gyroscope in accordance with the present invention.

FIG. 1B illustrates a second embodiment of a single axis gyroscope in accordance with the present invention.

FIG. 1C is a simple block diagram of the gyroscope of FIG. 1B.

FIG. 1D illustrates bode plots of the transfer functions Xdf/Fd and Xs/Fd of the gyroscope of FIG. 1B.

FIG. 2 illustrates a third embodiment of a single axis gyroscope in accordance with the present invention.

FIG. 3 illustrates a fourth embodiment of a single-axis gyroscope configuration in accordance with the present invention.

FIG. 4 illustrates a fifth embodiment of a single axis gyroscope in accordance with the present invention.

FIG. 5 illustrates a sixth embodiment of a single axis gyroscope in accordance with the present invention

FIG. 6 illustrates a seventh embodiment of a single axis gyroscope in accordance with the present invention.

FIG. 7 illustrates a single axis shear mode gyroscope in accordance with the present invention.

FIG. 8 illustrates a first embodiment of a tri-axis gyroscope in accordance with the present invention.

FIG. 9 illustrates a second embodiment of a tri-axis gyroscope in accordance with the present invention.

DETAILED DESCRIPTION

The present invention relates generally to angular velocity sensors and more particularly relates to angular velocity sensors that include guided mass systems. The following description is presented to enable one of ordinary skill in the art to make and use the invention and is provided in the context of a patent application and its requirements. Various modifications to the preferred embodiments and the generic principles and features described herein will be readily apparent to those skilled in the art. Thus, the present invention is not intended to be limited to the embodiments shown, but is to be accorded the widest scope consistent with the principles and features described herein.

FIG. 1A illustrates a first embodiment of a single axis gyroscope 100 a in accordance with the present invention. The single axis gyroscope is disposed in an X-Y plane parallel to a substrate 101 and comprises a drive system 110, a sense system 159 a and a coupling element 131. The drive system 110 includes a drive mass 130, an electrostatic actuator 109, two drive springs 105 a-b, an anchor 120 and two drive-sense electrodes 106 a-b. The drive springs 105 a-b and the anchor 120 act as a suspension system for the drive mass. The sense system 159 a comprises a rotating proof mass 150 a, a pivot spring 115, an anchor 140 and two capacitive sense electrodes 151 a and 151 b. Finally, the drive system 110 and the sense system 159 a are coupled by a coupling spring 131. In an embodiment, the suspension system is stiffer than the coupling spring 131 while the drive mass 130 is rotating out of plane.

The drive mass 130 is coupled to the substrate through spring elements 105 a-b and the anchor 120. In the drive operation of the single axis gyroscope 100 a, electrostatic forces are applied to the drive mass 130 via the electrostatic actuator 109, and the motion of drive mass 130 in Y direction is detected by electrostatic transducers 106 a and 106 b that are called drive-sense electrodes. The detected drive motion can be transferred to circuitry to be used to control the mechanical amplitude of drive mass 130 in a closed loop operation.

Although electrostatic actuators and transducers will be described throughout this specification, one of ordinary skill in the art recognizes that a variety of actuators could be utilized for this function and that use would be within the spirit and scope of the present invention. For example, the actuators or transducers could be piezoelectric, thermal or electromagnetic or the like.

The drive mass 130 is driven in the Y direction by the electrostatic actuator 109 at a certain frequency, which is referred to as a drive frequency. While drive mass 130 is driven in the Y direction, a moment around the Z-axis and a Y-direction force are applied to the rotating proof mass 150 a through the coupling spring 131. If the pivot spring 115 is very stiff in the Y direction, the rotating proof mass 150 a rotates around an axis that is parallel to the Z-axis due to the applied moment. The described motion of the drive mass 130 and rotating proof mass 150 a is referred to as a drive motion.

When the gyroscope 100 a is subject to an angular velocity about a roll-input axis in the Y-direction that is in the plane of the substrate 101 and orthogonal to the X-direction will cause Coriolis forces to act on the rotating proof mass 150 a in the Z-direction. The Coriolis forces cause the rotating proof mass 150 a to rotate out-of-plane about the roll-sense axis which is parallel to the X-direction. The amplitude of the rotation of the rotating proof mass 150 a is proportional to the angular velocity about the roll-input axis and also mechanical drive amplitude of the rotating proof mass 150 a. The capacitive sense electrodes 151 a and 151 b, which are placed on the substrate 101 under the rotating proof mass 150 a, are used to detect the rotation of the rotating proof mass 150 a about the roll-sense axis. This rotation provides a measure of the angular velocity about the roll-input axis. Although the capacitive electrodes 151 a and 151 b are given as transducers to detect the rotation of the rotating proof mass 150 a around the roll-sense axis, various types of transducers could be utilized in the present invention. For example, the capacitive electrodes 151 a-b could be also piezoelectric or optical or the like and its use would be within the spirit and scope of the present invention.

As it is given in FIGS. 1A and 1B, the drive mass 130 is separated from the rotating proof mass 150 a and the electrostatic actuators 109 are attached to the drive mass 130. A benefit of this approach is to eliminate the effect of the non-idealities of the electrostatic actuator 109 on the rotating proof mass 150 a. The non-idealities of the electrostatic actuator may be due to the fabrication imperfections, like sidewall angle during deep reactive ion etching, or built-in stresses due to the environmental effects.

As an example, the electrostatic forces generated by a non-ideal electrostatic actuator may not be only in-plane but also out-of plane, the out-of plane non-ideal forces could result in unwanted out-of plane motion and rotation of the rotating proof mass 150 a around its sensitive axis. The unwanted rotation of the rotating proof mass 150 a around its sensitive axis would lead to erroneous motion which can be detected by the capacitive sense electrodes 151 a-b resulting in an error in the measurement of angular velocity.

On the other hand, in FIGS. 1A and 1B, drive mass 130 is coupled to the anchor 120 via springs 105 a-b which are very stiff in Z direction. As a result, the motion of drive mass 130 due to the non-ideal out-of plane electrostatic forces by actuator 109 is minimized. Consequently, the non-ideal forces are not transferred to the proof mass 150 a, and measurement errors are reduced.

In FIG. 1A, the coupling spring 131, which is used to transfer the linear Y direction motion of the drive mass 130 to the rotation of the proof mass 150 a, can be made very stiff in Y-direction, but act as a pivot for rotation about z-axis or a torsion spring. Using a flexure as a coupling spring 131 in embodiment 100 a can be an option to satisfy those compliance conditions.

If the coupling spring 131 is made very stiff in Y-direction, but act as a pivot for rotation about z-axis, the whole single axis gyroscope 100 a would act as a single Degree of Freedom (DOF) mechanical system in the drive motion. The Y-direction motion of drive mass 130 is converted to in-plane rotation of the proof mass 150 a around an axis parallel to the Z direction. The amount of rotation of proof mass 150 depends on the ratio of the length of the coupling spring to the radius of rotation of the proof mass 150 a with respect to the center of its rotation. The Y-direction motion is either amplified or attenuated depending on the ratio. Moreover, the drive-sense electrodes 106 a-b can be placed on the drive mass 130 without effecting the closed loop drive operation.

FIG. 1B illustrates a second embodiment of a single axis gyroscope in accordance with the present invention. In the embodiment shown in FIG. 1B, the coupling spring 131 is compliant in the Y-direction and can be designed so that single axis gyroscope 100 b acts as a two DOF system in the drive motion. In that configuration, the sense system 159 b can be designed as a vibration absorber of the drive mass 130. As a result, small motion on drive mass 130 can be amplified to get bigger motion on the sense mass 150 a. For a vibration absorber configuration, it is necessary that drive-sense electrodes 106 a-b to be connected to the rotating proof-mass 150 a as it is shown in FIG. 1B. The connection is necessary to allow the rotational motion of rotating proof mass 150 a at a certain mechanical amplitude around the Z axis (the main component of the drive motion) to maximize the sensitivity of the gyroscope 100 b.

The small motion on the drive mass 130 is beneficial for area optimization. If the drive mass 130 has small drive motion, the electrostatic actuator gaps could be kept small, which will result in area savings. Moreover, the small drive motion is beneficial to minimize the spring softening, squeeze film damping and the non-linearity effects.

To explain the operation of the gyroscope 100 b in more detail refer now to FIGS. 1C and 1D. FIG. 1C is a simple block diagram of the gyroscope 100 b, the reference numerals which conform to those of FIG. 1B. It is desirable in the gyroscope 100 b that the drive mass 130 moves less than the sense mass 150 a. The minimization of motion of 130 is accomplished by tuning the coupling spring kc (131) such that it is at least an order of magnitude more flexible than the springs kd (105 a/105 b) and ks (115).

To explain the tuning of kc spring in more detail, bode plots of the transfer functions Xd/Fd and Xs/Fd are shown in FIG. 1D where Xd is the movement of the drive mass 130 in a first direction, Xs is the movement the sense mass 150 a in a second direction and Fd is the force caused by the actuator 109 on the drive mass 130. In FIG. 1D, the top plot shows the amplitude vs. frequency information and the bottom plot shows phase vs. frequency.

Xd/Fd transfer function has two peaks, and one zero. A first peak represents a motion of the drive mass (md) in the common mode shape, and the second peak represents a motion of the drive mass (md) in differential mode shape. In an embodiment, the flexibility of the coupling spring kc is such that the transfer function Xs/Fd is greater than Xd/Fd at a specific frequency range of interest. As an example in FIG. 1D, an expansion of a specific region has been shown. Based on the 2-DOF mechanical system dynamics, if the kc spring is sufficiently compliant compared to the ks and kd, the separation between first peak and zero is minimized in Xd/Fd transfer function. So, the amplitude of the first peak is attenuated. On the other hand Xs/Fd transfer function is not affected by the zero due to the 2-DOF system characteristics and its amplitude remains constant in the frequency range of interest. As a result, by placing the zero close to the first peak in Xd/Fd, the amplitude difference between drive mass and sense mass is obtained.

FIG. 2 illustrates a third embodiment of a single axis gyroscope 200 in accordance with the present invention. In this embodiment, the sense system 160 has some differences compared to the sense system 159 a which is shown in FIG. 1A. The sense system 160 comprises a circular proof mass 150 b, instead of a rectangular proof mass 150 a given in FIG. 1A. Moreover, the proof mass 150 b is coupled to the substrate via two pivot springs 115 a and 115 b and the anchor 141. The drive system 110 is similar to the embodiment given in FIG. 1A. Similar to the single axis gyroscopes shown in FIGS. 1A and 1B, the single axis gyroscope 200 is driven via electrostatic actuator 109 attached to the drive mass 130.

When the drive mass 130 is driven in Y direction, the proof mass 150 b rotates around Z axis. The amplitude of the drive motion of the proof mass 150 b depends on the drive mass 130 motion and the coupling spring 131 stiffness as it was explained previously. The amplitude of drive motion of the proof mass 150 b is detected by the drive sense electrodes 106 a and 106 b

An angular velocity about a roll-input axis in the Y-direction that is in the plane of the substrate 101 and orthogonal to the X-direction will cause Coriolis forces to act on the proof mass 150 b in the Z-direction. The Coriolis forces cause the proof mass 150 b to rotate out-of-plane about the roll-sense axis which is parallel to the X-direction. The amplitude of the rotation of the proof mass 150 b is proportional to the angular velocity about the roll-input axis. The capacitive sense electrodes 151 a and 151 b, which are placed on the substrate 101 under the proof mass 150 b, are used to detect the rotation of the proof mass 150 b about the roll-sense axis. This rotation provides a measure of the angular velocity about the roll-input axis.

FIG. 3 illustrates a fourth embodiment of a single-axis gyroscope 300 configuration in accordance with the present invention. The gyroscope configuration 300 includes two drive systems 110 a and 110 b, two coupling springs 131 a and 131 b, a rotating structure 161 and two yaw proof mass systems 180 a and 180 b. Drive systems 110 a and 110 b are similar to the drive system 110 given in FIG. 1A, FIG. 1B and FIG. 2. Drive systems 110 a-b both include anchors 120 a-b, drive springs 105 a-d, drive masses 130 a-b, drive-sense combs 106 a and 106 b and electrostatic actuators 109 a-b. Yaw proof mass systems 180 a-b both include a yaw proof mass 170 a-b, yaw sense springs 171 a-d and the electrostatic transducers 522 a-b.

Rotating structure 161 is coupled to the anchor 141 via springs 115 a-d. Rotating structure 161 is connected to the drive systems 110 a-b via coupling springs 131 a-b and finally rotating structure supports the yaw proof mass systems 180 a-b via springs 171 a-d. In the drive motion of the single-axis gyroscope 300, electrostatic actuators 109 a-b drives the proof masses 130 a and 130 b anti-phase in Y direction. Anti-phase motion of drive masses 130 a-b result in rotation of rotating structure 161 around Z-axis which is detected by the drive-sense combs 106 a and 106 b. As a result of the Z axis rotation of rotating structure 161, yaw proof masses 170 a-b translate anti-phase in the X direction since they are attached to rotating structure 161 through springs 171 a-d. Springs 171 a-d are very stiff in the X direction so that they don't deflect during the drive motion.

While the yaw proof masses are driven in X direction, an angular velocity about a yaw input axis in the Z direction that is normal to the substrate 101 will cause Coriolis forces to act on yaw proof masses 170 a-b in the Y-direction. The Coriolis forces cause the proof masses 170 a-b to translate anti-phase in Y direction. The amplitude of the rotation of the proof masses is proportional to the angular velocity about the yaw-input axis. The capacitive in-plane sense electrodes 522 a and 522 b, which are attached to the substrate 101 via anchors, are used to detect the Y direction translation of the proof masses 170 a-b. This translation provides a measure of the angular velocity about the yaw-input axis.

In FIG. 3, springs 115 a-d are configured such a way that the out of plane rotation and translation of rotating structure 161 is minimized. As a result, single-axis gyroscope 300 is not responsive to Coriolis forces around pitch and roll-input axes. However, for different embodiments, the spring configuration can be adjusted to detect the Coriolis response due to pitch and roll axes inputs.

The drive systems 110 a and 110 b are decoupled from the yaw proof masses 170 a and 170 b by using a similar approach given in FIG. 1A. Consequently, the benefits of decoupling the drive system from the sensing proof mass mentioned in the explanation of FIGS. 1A and 1B will apply equally to the single-axis gyroscope 300.

FIG. 4 illustrates a fifth embodiment of a single axis gyroscope 400 in accordance with the present invention. In the gyroscope 400, a guided mass system 401 is disposed in an X-Y plane parallel to a substrate 101. The guided mass system 401 includes guiding arms 104 a and 104 b that are flexibly coupled via springs 108 a and 108 b to the substrate 101 via the anchoring points 142 a and 142 b, respectively. The two guiding arms 104 a and 104 b are flexibly coupled to the roll proof-masses 200 a-b via springs 103 a-d.

The roll proof-masses 200 a-b, guiding arms 104 a and 104 b, anchoring points 142 a-b, and springs 103 a-d, 108 a-b form a planar four-bar linkage. Each spring 103 a-d and 108 a-b is compliant in-plane about an axis in the Z-direction so that each guiding arm 104 a and 104 b can rotate in-plane while the proof-masses 200 a-b translates anti-phase in an X-direction.

The springs 108 a and 108 b are compliant about a first roll-sense axis in the X-direction so that the guiding arms 104 a and 104 b can rotate out-of-plane. The springs 103 a-d are stiff in the Z-direction, whereby out-of-plane rotation of the guiding arms 104 a and 104 b causes the roll proof-masses 200 a-b to move anti-phase out-of-plane.

Drive systems 110 a and 110 b are similar to the drive system 110 described with respect to FIG. 3. Drive systems 110 a-b both include anchors 120 a-b, drive springs 105 a-d, drive masses 130 a-b, drive-sense combs 106 a and 106 b and electrostatic actuators 109 a-b and they are coupled to guiding arms 104 a and 104 b via coupling springs 131 a and 131 b.

The guided mass system 401 can be driven at a drive frequency by a single drive circuit coupled to the actuators 109 a and 109 b. The drive frequency can be a resonant frequency of the single-axis gyroscope 400. When the drive masses 130 a-b are driven anti-phase in the Y direction with the electrostatic force applied by the actuators 109 a-b, the guiding arms 104 a and 104 b rotate in-plane and the roll proof-masses 200 a-b translates in-plane anti-phase in the X-direction which is detected by the drive-sense combs 106 a and 106 b.

Angular velocity about a roll-input axis in the Y-direction that is in the plane of the substrate and orthogonal to the X-direction will cause Coriolis forces to act on the roll proof-masses 200 a-b in the Z-direction. The Coriolis forces cause the guided mass system 401 to rotate out-of-plane about the first roll-sense axis which is parallel to the X-direction. When the guided mass system 401 rotates out-of-plane, the guiding arms 104 a and 104 b and the roll proof-masses 200 a-b rotate out-of-plane about the first roll-sense axis.

The amplitude of the rotation of the guided mass system 401 is proportional to the angular velocity about the roll-input axis. Transducers 201 a-b under the roll proof-masses 200 a-b are used to detect the rotation of the guided mass system 401 about the roll-sense axis. This rotation provides a measure of the angular velocity about the roll-input axis.

FIG. 5 illustrates a sixth embodiment of a single axis gyroscope 500 in accordance with the present invention In the gyroscope 500, a guided mass system 501 comprises guided proof masses 200 a-b, guiding arm 104 a, and pitch proof mass 210. Single axis gyroscope further comprises drive system 110, which is similar to the drive system given in FIG. 1A. Drive system 110 is coupled to the guided mass system 501 via coupling spring 131. Guiding arm 104 a is connected to substrate 101 via spring 108 a through anchor 142 a. Guided proof masses 200 a and 200 b are coupled to guiding arm 104 a via springs 103 a and 103 c, respectively. Furthermore, guided proof masses 200 a-b are coupled to the substrate via springs 119 a-b through anchor 143.

The pitch proof-mass 210 is flexibly connected to two guided proof-masses 200 a and 200 b via springs 210 a and 210 b, respectively. Springs 210 a and 210 b are torsionally compliant such that pitch proof-mass 210 can rotate out-of-plane about a pitch sense axis in the Y-direction. During the drive motion of single axis gyroscope 500, drive mass 130 is driven in Y direction by actuator 109. The Y direction motion is transferred to the guided mass system through coupling spring 131 and results in rotation of guiding arm 104 a about an axis that is parallel to the Z direction. The in-plane rotation of guided arm 104 a causes anti-phase translation of guided proof masses 200 a-b in the X direction. Springs 210 a and 210 b are compliant in-plane such that when the guided proof-masses 200 a and 200 b are driven anti-phase in the X-direction; the pitch proof-mass 210 rotate in-plane about an axis in the Z-direction.

Angular velocity about the pitch-input axis will cause Coriolis forces to act on the pitch proof-mass 210 resulting in a torque that rotates the pitch proof-mass 210 about the pitch-sense axis. The amplitude of the rotation of the pitch proof-mass 210 is proportional to the angular velocity about the pitch-input axis. Transducers 211 a and 211 b are disposed on opposite sides along the X-direction under the pitch proof-mass 210 and detect the rotation of the pitch proof-mass about the pitch-sense axis. This rotation provides a measure of the angular velocity about the pitch-input axis.

FIG. 6 illustrates a seventh embodiment of a single axis gyroscope 600 in accordance with the present invention. Single axis gyroscope 600 includes a guided mass system 601 coupled to two yaw proof masses 170 a and 170 b and a drive system 110.

Drive system 110 is coupled to the guided mass system 601 via coupling spring 131. Guiding arm 104 a is connected to substrate 101 via spring 108 a through anchor 142 a. Guided proof masses 200 a and 200 b are coupled to guiding arm 104 a via springs 103 a and 103 c, respectively. Furthermore, guided proof masses 200 a-b are coupled to the substrate via springs 119 a-b through anchor 143.

The yaw proof-masses 170 a and 170 b are flexibly connected to guided proof masses 200 a and 200 b via springs 171 a-b and 171 c-d respectively. Springs 171 a-d are compliant in Y direction such that yaw proof-masses 170 a and 170 b can translate along an axis parallel to the Y direction. During the drive motion of single axis gyroscope 600, drive mass 130 is driven in Y direction by actuator 109. The Y direction motion is transferred to the guided mass system through coupling spring 131 and results in rotation of guiding arm 104 a about an axis that is parallel to the Z direction. The in-plane rotation of guided arm 104 a causes anti-phase translation of guided proof masses 200 a-b in the X direction. Springs 171 a-d are axially stiff in the X-direction such that when the guided proof-masses 200 a and 200 b are driven anti-phase in the X-direction, the yaw proof-masses 170 a and 170 b also translate anti-phase in the X-direction.

Angular velocity about the yaw-input axis will cause Coriolis forces to act on the yaw proof-masses 170 a and 170 b resulting in motion of the yaw proof-masses 170 a-b anti-phase along the Y-direction. The amplitude of the motion of the yaw proof masses along the Y-direction is proportional to the angular velocity. Transducers 522 a and 522 b are used to sense the motion of the respective yaw proof masses 170 a and 170 b along the Y-direction.

FIG. 7 illustrates a single axis shear mode gyroscope 700 in accordance with the present invention. Gyroscope 700 includes shear masses 200 a and 200 b which are coupled to a substrate 101 via spring elements 119 a-b and 119 c-d through anchors 143 a and 143 b. Drive systems 110 a-b are connected to the shear proof masses 200 a and 200 b via coupling springs 131 a and 131 b, respectively. The pitch proof-mass 210 is flexibly connected to two shear masses 200 a and 200 b via springs 210 a and 210 b. Springs 210 a and 210 b are torsionally compliant such that pitch proof-mass 210 can rotate out-of-plane about a pitch sense axis in the Y-direction.

Each drive system 110 a and 110 b of FIG. 7 includes a drive mass 130 a-b which are coupled to the substrate via drive springs 105 a-b and 105 c-d through the anchors 120 a-b. In the drive motion of single axis shear mode gyroscope 700, the drive masses 130 a-b are driven anti-phase in the X direction by the actuators 109 a and 109 b. X direction motion of the drive masses 130 a-b is transferred to the shear masses 200 a-b via the coupling springs 131 a-b. As a result, the shear masses 200 a-b are driven anti-phase in the X-direction. Springs 210 a and 210 b are compliant in-plane such that when the shear masses 200 a and 200 b are driven anti-phase in the X-direction; the pitch proof-mass 210 rotate in-plane about an axis in the Z-direction.

Drive motion of the shear masses 200 a and 200 b is referred to hereinafter as shear mode drive motion. Shear mode drive motion can be generalized by defining a specific motion between the two shear masses 200 a and 200 b and their coupling relationship. In the shear mode drive motion, the two shear masses 200 a and 200 b are coupled with a spring or spring-mass system, and the shear masses 200 a and 200 b translate anti-phase along a direction that is perpendicular to a line that is connecting their geometric center.

Angular velocity about the pitch-input axis will cause Coriolis forces to act on the pitch proof-mass 210 resulting in a torque that rotates the pitch proof-mass 210 about the pitch-sense axis. The amplitude of the rotation of the pitch proof-mass 210 is proportional to the angular velocity about the pitch-input axis. Transducers 211 a and 211 b are disposed on opposite sides along the X-direction under the pitch proof-mass 210 and detect the rotation of the pitch proof-mass about the pitch-sense axis. This rotation provides a measure of the angular velocity about the pitch-input axis.

FIG. 8 illustrates a first embodiment of a tri-axis gyroscope 800 in accordance with the present invention. The gyroscope 800 includes two guided mass systems 801 and 802 coupled together by a coupling spring 302 which connects roll proof-masses 200 b and 200 c. Guided mass system 801 comprises guided roll proof-masses 200 a-b, guiding arms 104 a-b, and yaw proof-masses 170 a-b. The yaw proof-masses 170 a and 170 b are flexibly connected to the roll proof-masses 200 a and 200 b via springs 171 a-b and 171 c-d respectively. Guided mass system 802 comprises guided roll proof-masses 200 c-d, guiding arms 104 c-d, and a pitch proof mass 210. The pitch proof-mass 210 is flexibly connected to two guided proof-masses 200 a and 200 b via springs 210 a and 210 b, respectively. Springs 210 a and 210 b are torsionally compliant such that pitch proof-mass 210 can rotate out-of-plane about a pitch sense axis in the Y-direction. Drive systems 110 a and 110 b are coupled to the guided mass system 801 through guiding arms 104 a and 104 b via coupling springs 131 a and 131 b. In different embodiments of tri-axis gyroscope 800, drive systems 110 a-b can also be coupled to guided mass system 802.

Tri-axis gyroscope 800 is driven at a drive frequency by a single drive circuit (not shown) coupled to the actuators 109 a-b. The drive masses 130 a-b are vibrated anti-phase in the Y direction with the electrostatic force applied by the actuators 109 a-b. Motion of the drive masses 130 a-b transferred to the guiding arms 104 a and 104 b through the coupling springs 131 a and 131 b. Guiding arms 104 a and 104 b rotate in-plane around an axis that is parallel to the Z direction due to the applied torque which is a result of the motion of the drive masses 130 a-b. As a result of the in-plane rotation of guiding arms 104 a and 104 b, the roll proof-masses 200 a-b translates in-plane anti-phase in the X-direction. Springs 171 a-d are axially stiff in the X-direction such that when the roll proof-masses 200 a and 200 b are driven anti-phase in the X-direction, the yaw proof-masses 170 a and 170 b also translate anti-phase in the X-direction.

The coupling spring 302 is stiff in the X-direction such that roll proof-masses 200 b and 200 c move together in the X-direction. The roll proof-masses 200 a and 200 d move in opposite direction of roll proof-masses 200 b and 200 c. Springs 210 a and 210 b are compliant in-plane such that when the roll proof-masses 200 c-d are driven, the pitch proof-mass 210 rotate in-plane about an axis parallel to the Z-direction.

Angular velocity about the pitch-input axis will cause Coriolis forces to act on the pitch proof-mass 210 resulting in a torque that rotates the pitch proof-mass 210 about the pitch-sense axis. The amplitude of the rotation of the pitch proof-mass 210 is proportional to the angular velocity about the pitch-input axis. Transducers 211 a and 211 b are disposed on opposite sides along the X-direction under the pitch proof-mass 210 and detect the rotation of the pitch proof-mass about the pitch-sense axis. This rotation provides a measure of the angular velocity about the pitch-input axis.

Angular velocity about the roll-input axis causes Coriolis forces to act on the roll proof-masses 200 a-d in the positive and negative Z-direction. The coupling spring 302 is torsionally compliant about an axis in the X-direction so that the guided mass systems 801 and 802 can rotate anti-phase out-of-plane about the first and second roll-sense axes. The coupling spring 302 is stiff in the Z-direction which prevents the guided mass systems 801 and 802 from rotating in-phase out-of-plane. Transducers 201 a-c under the roll proof masses 200 a-d are used to detect the rotations of the guided mass systems 801 and 802 about the first and second roll-sense axes.

Angular velocity about the yaw-input axis will cause Coriolis forces to act on the yaw proof-masses 170 a and 170 b resulting in motion of the yaw proof-masses 170 a and 170 b anti-phase along the Y-direction. The amplitude of the motion of the yaw proof-masses along the Y-direction is proportional to the angular velocity. Transducers 522 a and 522 b are used to sense the motion of the respective yaw proof masses 170 a and 170 b along the Y-direction.

FIG. 9 illustrates a second embodiment of a tri-axis gyroscope 900 in accordance with the present invention. Tri-axis gyroscope 900 comprises three guided mass systems 901, 902, 903 and two drive mass systems 110 a-b. Guided mass systems 901 and 903 are coupled to guided mass system 902 by coupling springs 302 a and 302 b. And drive mass systems 110 a and 110 b are coupled to the guided mass system 902 via coupling springs 131 a and 131 b.

The guided mass systems 901, 902 and 903 are arranged so that the roll proof-masses 200 a-d all move in the X-direction, the pitch proof-mass 210 rotates about an axis in the Z-direction, and the yaw proof-masses 170 a and 170 b move anti-phase in the X-direction. The guided mass system 901 rotates out-of-plane about a first roll-sense axis. The guided mass system 902 rotates out-of-plane about a second roll-sense axis parallel to the first roll-sense axis. The guided mass system 903 rotates out-of-plane about a third roll-sense axis parallel to the first and second roll-sense axes.

The first coupling spring 302 a is connected to roll proof-masses 200 b and 200 c. The coupling spring 302 a is stiff in the X-direction such that roll proof-mass 200 b and 200 c move together in the X-direction. The second coupling spring 302 b is connected to roll proof-masses 200 a and 200 d. The coupling spring 302 b is stiff in the X-direction such that roll proof-mass 200 a and 200 d move together in the X-direction. In this way the guided mass systems 901, 902, and 903 are driven together at a drive frequency by a single drive circuit coupled to the actuators 109 a-b. During the drive motion, drive masses 130 a-b are vibrated anti-phase in the Y direction with the electrostatic force applied by the actuators 109 a-b. Motion of the drive masses 130 a-b transferred to the guiding arms 104 a and 104 b through the coupling springs 131 a and 131 b, and the guiding arms 104 a-b rotate in-plane around an axis that is parallel to the Z direction. As a result of the in-plane rotation of guiding arms 104 a and 104 b, the roll proof-mass pair 200 b and 200 c and roll proof-mass pair 200 a and 200 d translate anti-phase in-plane in the X-direction which is detected by the drive-sense combs 106 a, 106 b, 106 c, and 106 d.

Moreover, during the drive motion, the guided mass systems 901, 902 and 903 are arranged so that when the roll proof-masses 102 a-d all move in the X-direction, the pitch proof-mass 210 rotates about an axis in the Z-direction, and the yaw proof-masses 170 a and 170 b move anti-phase in the X-direction.

The coupling spring 302 a is torsionally compliant about an axis in the X-direction so that the guided mass systems 901 and 902 can rotate out-of-plane about the first and second roll-sense axes anti-phase. The coupling spring 302 a prevents the symmetric guided mass systems 901 and 902 from rotating out-of-plane in-phase.

The coupling spring 302 b is also torsionally compliant about an axis in the X-direction so that the guided mass systems 902 and 903 can rotate out-of-plane about the second and third roll-sense axes anti-phase. The coupling spring 302 b prevents the symmetric guided mass systems 902 and 903 from rotating out-of-plane in-phase.

Angular velocity about the pitch-input axis will cause Coriolis forces to act on the pitch proof-mass 210 resulting in a torque that rotates the pitch proof-mass 210 about the pitch-sense axis. The amplitude of the rotation of the pitch proof-mass 210 is proportional to the angular velocity about the pitch-input axis. Transducers 211 a and 211 b are disposed on opposite sides along the X-direction under the pitch proof-mass 210 and detect the rotation of the pitch proof-mass about the pitch-sense axis. The rotation provides a measure of the angular velocity about the pitch-input axis.

Angular velocity about the roll-input axis will cause Coriolis forces to act on the roll proof-masses 200 b and 200 c in a Z-direction and on roll proof-masses 200 a and 200 d in the opposite Z-direction. The Coriolis forces cause the guided mass systems 901, 902, and 903 to rotate out-of-plane about the first, second, and third roll-sense axis respectively. Transducer 201 a under the roll proof masses 200 b and 102 c and transducer 201 a under the roll proof masses 200 a and 200 d are used to detect the rotation of the guided mass systems 901,902 and 903. This rotation provides a measure of the angular velocity about the roll-input axis.

Angular velocity about the yaw-input axis will cause Coriolis forces to act on the yaw proof-masses 170 a and 170 b resulting in motion of the yaw proof-masses 170 a and 170 b anti-phase along the Y-direction. The amplitude of the motion of the yaw proof-masses along the Y-direction is proportional to the angular velocity. Transducers 522 a and 522 b are used to sense the motion of the respective yaw proof masses 170 a and 170 b along the Y-direction.

CONCLUSION

In all of the above embodiments of the gyroscope, the drive mass is separated from the rotating proof mass and the electrostatic actuators are attached to the drive mass. In so doing, the effect of the non-idealities of the electrostatic actuator on the rotating proof mass is minimized thereby enhancing the overall sensitivity of the gyroscope.

Although the present invention has been described in accordance with the embodiments shown, one of ordinary skill in the art will readily recognize that there could be variations to the embodiments and those variations would be within the spirit and scope of the present invention. Accordingly, many modifications may be made by one of ordinary skill in the art without departing from the spirit and scope of the present invention. 

What is claimed is:
 1. An angular rate sensor comprising; a substrate; a rotating structure coupled to the substrate; a drive mass coupled to the substrate; a flexible element coupling the drive mass and the rotating structure; an actuator coupled to the rotating structure via the drive mass for driving the rotating structure into rotational oscillation around a first axis normal to the substrate; a first transducer responsive to the rotational oscillation of the rotating structure during a drive mode; and a second transducer which is responsive to the angular velocity of the angular rate sensor.
 2. The angular rate sensor of claim 1, wherein the first transducer is attached to the rotating structure.
 3. The angular rate sensor of claim 1, wherein the rotating structure comprises any of a rectangular proof mass or a circular proof mass.
 4. The angular rate sensor of claim 1, wherein the drive mass is driven in a translational mode.
 5. The angular rate sensor of claim 1, wherein an amplitude of the rotating structure is dependent upon the drive mass motion and the coupling element stiffness.
 6. The sensor of claim 1, wherein at least one first proof mass is flexibly coupled to the rotating structure and the at least one first proof mass responds to a Coriolis force.
 7. The sensor of claim 1, wherein the rotating structure responds to a Coriolis force.
 8. The sensor of claim 1, wherein the rotating structure is flexibly coupled to an at least one first translational mass and wherein the first translational mass is flexibly coupled to the substrate and translates along a second axis which is parallel to the substrate.
 9. The angular rate sensor of claim 8, wherein the first transducer is attached to the first translational mass.
 10. The sensor of claim 8, includes a second translational mass, wherein the second translational mass is flexibly coupled to the substrate and translates along a third axis which is parallel to the substrate and to the second axis and wherein the first and second translational mass moves out of phase along the second and the third axis, respectively.
 11. The sensor of claim 10, wherein the first and second translational masses are able to move anti-phase in response to a Coriolis force acting in a direction that is normal to the substrate generated by an angular rate around a fourth axis that is in-plane and orthogonal to the second axis.
 12. The sensor of claim 5, wherein the drive mass and the rotating structure forms a mechanical system with two-degrees of freedom.
 13. The sensor of claim 12, wherein motion of the drive mass is less than the motion of the rotating structure.
 14. The sensor of claim 8, wherein a proof mass is flexibly connected to the first translational mass via a first spring and flexibly connected to the second translational mass via a second spring and rotates around an axis orthogonal to the substrate while the drive mass is driven in a first direction.
 15. The sensor of claim 14, wherein the proof mass responds to a Coriolis force generated by an angular rate around an axis parallel to the substrate and orthogonal to the first axis.
 16. The sensor of claim 10, wherein a proof mass is flexibly connected to the first translational mass which is able to move in the same direction as the second translational mass.
 17. The sensor of claim 16, wherein a second proof mass is flexibly connected to a second translational mass which is able to move in the same direction as the first translational mass.
 18. The sensor of claim 16, wherein the proof masses is able to move in response to a Coriolis force acting in a direction that is parallel to the first axis generated by an angular rate around an axis that is orthogonal to the substrate.
 19. The sensor of claim 1, further comprising a suspension system coupling the drive mass to the substrate, wherein the suspension system is stiffer than the flexible element while rotating out of plane.
 20. An angular rate sensor comprising; a substrate; a first and second shear masses coupled to the substrate; a drive mass coupled to the substrate; a flexible element coupling the drive mass and the first and second shear masses; an actuator coupled to and the first and second shear masses via the drive mass for driving the and the first and second shear masses into anti-phase oscillation along a first and second direction parallel to each other; a first transducer responsive to the anti-phase oscillation during a drive mode; and a second transducer which is responsive to the angular velocity of the angular rate sensor.
 21. The sensor of claim 20, wherein the first transducer is attached to the shear mass.
 22. The sensor of claim 20, wherein the first and second shear masses are coupled to each other.
 23. The sensor of claim
 20. wherein the drive mass and the first and second shear masses forms a mechanical system with two-degrees of freedom and wherein motion of the drive mass is less than the motion of the first and second proof masses.
 24. The sensor of claim 20, wherein the first and second shear masses are flexibly coupled to a first translational mass and wherein the first translational mass is flexibly coupled to the substrate and translates along a second axis which is parallel to the substrate.
 25. The sensor of claim 24, wherein a proof mass is flexibly connected to the first translational mass via a first spring and flexibly connected to a second translational mass via a second spring and rotates around an axis orthogonal to the substrate while the drive mass is driven in a first direction.
 26. The sensor of claim 25, wherein a second proof mass is flexibly connected to the first translational mass which is able to move in the same direction as the second translational mass. 